The Mesoscale Organization of Deep Convection

The organization of systems at all scales has long been an observed feature in meteorology. Coherent structures can be found from eddies in the planetary boundary layer up to tropical cyclones and mid-latitude depressions. The problem of organization is thus of a fundamental nature. An understanding of the organization of deep convection is relevant to this general problem but is complicated by the three-phase physics of water. The phase changes play a fundamental role in convection, not only in producing hydrometeors, but in strongly influencing the internal dynamics through the buoyant force.

[1]  Edward J. Zipser,et al.  Mesoscale and convective-scale downdrafts as distinct components of squall-line structure , 1977 .

[2]  Yukari N. Takayabu,et al.  Large-Scale Cloud Disturbances Associated with Equatorial Waves, Part I: Spectral Features of the Cl , 1994 .

[3]  G. M. Barnes,et al.  The Environment of Fast- and Slow-Moving Tropical Mesoscale Convective Cloud Lines , 1984 .

[4]  A. Numaguti Characteristics of 4-to-20-Day-Period Disturbances Observed in the Equatorial Pacific during the TOGA COARE IOP , 1995 .

[5]  J. Lafore,et al.  The West African Squall Line Observed on 23 June 1981 during COPT 81: Mesoscale Structure and Transports , 1988 .

[6]  Yukari N. Takayabu,et al.  Large-Scale Cloud Disturbances Associated with Equatorial Waves: Part II: Westward-Propagating Inertio-Gravity Waves@@@Part II 西進慣性重力波 , 1994 .

[7]  Donald C. Norquist,et al.  The Structure and Properties of African Wave Disturbances as Observed During Phase III of GATE , 1977 .

[8]  Mitchell W. Moncrieff,et al.  A Numerical Investigation of the Organization and Interaction of the Convective and Stratiform Regions of Tropical Squall Lines , 1988 .

[9]  Properties of African squall lines inferred from time-lapse satellite imagery. , 1980 .

[10]  J. Lafore,et al.  African Easterly Waves and Convection. Part I: Linear Simulations , 1995 .

[11]  W. Tao,et al.  Modeling Study of a Tropical Squall-Type Convective Line , 1989 .

[12]  J. Lafore,et al.  Equatorial Atmospheric Waves and Their Association to Convection , 1997 .

[13]  F. Roux The West African Squall Line Observed on 23 June 1981 during COPT 81: Kinematics and Thermodynamics of the Convective Region , 1988 .

[14]  M. Chong,et al.  A Tropical Squall Line Observed during the COPT 81 Experiment in West Africa. Part II: Water Budget , 1989 .

[15]  Jean-Luc Redelsperger,et al.  Comparison between a Three-Dimensional Simulation and Doppler Radar Data of a Tropical Squall Line: Transports of Mass, Momentum, Heat, and Moisture , 1988 .

[16]  M. Desbois,et al.  Characterization of Some Elements of the Sahelian Climate and Their Interannual Variations for July 1983, 1984 and 1985 from the Analysis of METEOSAT ISCCP Data , 1988 .

[17]  Joseph B. Klemp,et al.  A Study of the Tornadic Region within a Supercell Thunderstorm , 1983 .

[18]  Mitchell W. Moncrieff,et al.  Two‐dimensional convection in non‐constant shear: A model of mid‐latitude squall lines , 1982 .

[19]  John D. Marwitz,et al.  The Structure and Motion of Severe Hailstorms. Part I: Supercell Storms , 1972 .

[20]  T. Matsuno,et al.  Quasi-geostrophic motions in the equatorial area , 1966 .

[21]  M. Lemone,et al.  Vertical velocity in oceanic convection off tropical Australia , 1994 .

[22]  Alan K. Betts,et al.  The Thermodynamic Transformation of the Tropical Subcloud Layer by Precipitation and Downdrafts , 1976 .

[23]  J. Klemp,et al.  A Three-Dimensional Numerical Simulation of Splitting Severe Storms on 3 April 1964 , 1981 .

[24]  A. E. Gill Atmosphere-Ocean Dynamics , 1982 .

[25]  R. Houze,et al.  Rear Inflow in Squall Lines with Trailing Stratiform Precipitation , 1987 .

[26]  G. Caniaux,et al.  A Numerical Study of the Stratiform Region of a Fast-Moving Squall Line. Part I: General Description and Water and Heat Budgets , 1994 .

[27]  Mitchell W. Moncrieff,et al.  Organized convective systems : archetypal dynamical models, mass and momentum flux theory, and parametrization , 1992 .

[28]  Robert A. Houze,et al.  Radar Characteristics of Tropical Convection Observed During GATE: Mean Properties and Trends Over the Summer Season , 1977 .

[29]  M. E. Nicholls A Comparison of the Results of a Two-Dimensional Numerical Simulation of a Tropical Squall Line with Observations , 1987 .

[30]  G. Scialom,et al.  A Tropical Squall Line Observed during the COPT 81 Experiment in West Africa. Part 1: Kinematic Structure Inferred from Dual-Doppler Radar Data , 1987 .

[31]  Mitchell W. Moncrieff,et al.  The propagation and transfer properties of steady convective overturning in shear , 1972 .

[32]  R. Houze,et al.  Kinematic and Precipitation Structure of the 10–11 June 1985 Squall Line , 1991 .

[33]  Edward J. Zipser,et al.  Cumulonimbus Vertical Velocity Events in GATE. Part II: Synthesis and Model Core Structure , 1980 .

[34]  Joseph B. Klemp,et al.  Characteristics of Isolated Convective Storms , 1986 .

[35]  Y. Tourre,et al.  Some Climatological Aspects of West African Disturbance Lines During GATE , 1976 .

[36]  Michael I. Biggerstaff,et al.  Interpretation of Doppler Weather Radar Displays of Midlatitude Mesoscale Convective Systems , 1989 .

[37]  Robert A. Houze,et al.  Melting and Evaporation of Hydrometeors in Precipitation from the Anvil Clouds of Deep Tropical Convection , 1979 .

[38]  Mitchell W. Moncrieff,et al.  Organized convective systems in the tropical western pacific as a process in general circulation models: A toga coare case‐study , 1997 .

[39]  D. J. Musil,et al.  Structure of an Evolving Hailstorm Part V: Synthesis and implications for Hail Growth and Hail Suppression , 1976 .

[40]  Jean-Luc Redelsperger,et al.  A three-dimensional simulation of a tropical squall line: convective organization and thermodynamic vertical transport , 1988 .

[41]  W. Frank The Life Cycles of GATE Convective Systems , 1978 .

[42]  R. Dmowska,et al.  International Geophysics Series , 1992 .

[43]  F. Guichard,et al.  Thermodynamical impact and internal structure of a tropical convective cloud system , 1997 .

[44]  R. Houze,et al.  A Midlatitude Squall Line with a Trailing Region of Stratiform Rain: Radar and Satellite Observations , 1985 .

[45]  R. Carbone,et al.  A Preliminary Morphology of Precipitation Systems In Tropical Northern Australia , 1992 .

[46]  Modification of Surface Fluxes by Atmospheric Convection in the TOGA COARE Region , 1996 .

[47]  Edward J. Zipser,et al.  Momentum Flux by Lines of Cumulonimbus over the Tropical Oceans , 1984 .

[48]  F. Roux,et al.  Single-Doppler Observations of a West African Squall Line on 27-28 May 1981 during COPT 81: Kinematics, Thermodynamics and Water Budget , 1990 .

[49]  Brian E. Mapes,et al.  Multiscale variability of deep convection in relation to large-scale circulation in TOGA COARE , 1996 .

[50]  Robert G. Fovell,et al.  Numerical Simulation of a Midlatitude Squall Line in Two Dimensions , 1988 .

[51]  G. Caniaux,et al.  A Numerical Study of the Stratiform Region of a Fast-Moving Squall Line. Part II: Relationship between Mass, Pressure, and Momentum Fields , 1995 .

[52]  R. Rotunno,et al.  A Theory for Strong, Long-Lived Squall Lines , 1988 .